{"qid": "D3105", "reaction": "e- + H2 X(1\u03a3+g);v=10 \u2192 H2 e(3\u03a3+u) + e-", "process_types": {"EDE": "Dissociative Excitation"}, "data_type": "cross section", "refs": {"B10": {"doi": "10.1016/j.adt.2020.101361"}}, "comment": "MCCC calculations of vibrationally-resolved electron-impact dissociative excitation of H2, adiabatic nuclei calculations performed with the spheroidal MCCC(210) model", "method": "MCCC", "columns": [{"name": "E", "units": "eV"}, {"name": "sigma", "units": "cm2"}], "unc_perc": 10.0, "threshold": 10.8187, "fit": {"coeffs": {"A1": 0.049782, "A2": -0.031846, "A3": 0.57436, "A4": -0.1252, "A5": -0.3742}, "func": "singlet_triplet_H2"}, "data_from_fit": false, "metadata_version": "M1.0", "time_added": "2022-05-26 10:44:30.548788+00:00"}
------------------------------------------------------------------------
1.082e+01 0.0
1.150e+01 1.455e-19
1.200e+01 2.55e-19
1.250e+01 3.524e-19
1.300e+01 4.279e-19
1.350e+01 6.185e-19
1.400e+01 6.517e-19
1.450e+01 6.933e-19
1.500e+01 7.091e-19
1.550e+01 7.657e-19
1.600e+01 7.575e-19
1.650e+01 7.888e-19
1.700e+01 7.735e-19
1.750e+01 7.717e-19
1.800e+01 7.873e-19
1.850e+01 7.764e-19
1.900e+01 7.589e-19
1.950e+01 7.38e-19
2.000e+01 7.18e-19
2.100e+01 6.731e-19
2.200e+01 6.269e-19
2.300e+01 5.814e-19
2.400e+01 5.383e-19
2.500e+01 4.978e-19
2.600e+01 4.602e-19
2.700e+01 4.256e-19
2.800e+01 3.94e-19
2.900e+01 3.65e-19
3.000e+01 3.386e-19
3.500e+01 2.372e-19
4.000e+01 1.717e-19
4.500e+01 1.28e-19
5.000e+01 9.789e-20
6.000e+01 6.097e-20
7.000e+01 4.054e-20
8.000e+01 2.833e-20
9.000e+01 2.06e-20
1.000e+02 1.546e-20
1.250e+02 8.372e-21
1.500e+02 5.049e-21